The present analysis is based on tracking information from the Inner Tracking System (ITS) [1]} and the Time Projection Chamber (TPC) [2]}.
Both detectors are located within a large solenoidal magnet which provides a nominal field strength of 0.5 T for all of the data taking periods analysed in this work, except for the Xe==Xe data taking, where the magnetic field was reduced to 0.2 T in order to extend the kinematic acceptance of the detector to lower transverse momentum.
The ITS is comprised of six cylindrical layers of silicon detectors with radii between 3.9 cm and 43 cm.
Its two innermost layers are equipped with silicon pixel detectors (SPD), the two intermediate layers consist of silicon drift detectors (SDD), and the two outermost layers are made of double-sided silicon strip detectors (SSD).
The large cylindrical TPC has an active radial range from about 85 cm to 250 cm and an overall length along the beam direction of about 500 cm.
It covers the full azimuth in the pseudorapidity range \({|\eta | < 0.9}\)  and provides track reconstruction with up to 159 space points along the trajectory of a charged particle as well as particle identification via the measurement of specific energy loss \({\rm d}E/{\rm d}x\) .
The V0 detector, which consists of two scintillator arrays covering the pseudorapidity ranges of \({2.8<\eta <5.1}\)  (V0A) and \({-3.7<\eta <-1.7}\)  (V0C), is used for triggering on hadronic collisions and multiplicity measurements at forward rapidity [3]}, [4]}.
